2021
DOI: 10.1103/physrevd.103.103525
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Cosmological consequences of a principle of finite amplitudes

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Cited by 27 publications
(32 citation statements)
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“…15 Note that the case where w = −(1 + λ/2)/d corresponds to saturating the SEC, and from (A.7), it corresponds to Minkowski space in the Einstein frame. This is the basis of the loitering solution studied in [48,49,78]. 16 The only exception is when λ = −2, in which case it can be shown [47] that the solution H = H0 anḋ Φ = −βH0 is stable for any constant β > 0.…”
Section: Jhep07(2021)149mentioning
confidence: 96%
“…15 Note that the case where w = −(1 + λ/2)/d corresponds to saturating the SEC, and from (A.7), it corresponds to Minkowski space in the Einstein frame. This is the basis of the loitering solution studied in [48,49,78]. 16 The only exception is when λ = −2, in which case it can be shown [47] that the solution H = H0 anḋ Φ = −βH0 is stable for any constant β > 0.…”
Section: Jhep07(2021)149mentioning
confidence: 96%
“…where N, N i , (3) g ij denote respectively the lapse function, shift vector, and 3dimensional induced metric on the leaves. The theory is constructed from the following quantities:…”
Section: Horava-lifshitz Gravitymentioning
confidence: 99%
“…where (3) R ij is the 3-dimensional Ricci curvature tensor, (3) ∇ i is the covariant derivative constructed from the 3-dimensional metric (3) g ij , and a i := N,i N . Extrinsic curvature K ij is the only object, invariant under general spatial diffeomorphisms containing exactly one time derivative of the metric tensor (3) g ij :…”
Section: Horava-lifshitz Gravitymentioning
confidence: 99%
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